{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:U4ER4LNAWEVCID3NGRFZPIKNPT","short_pith_number":"pith:U4ER4LNA","schema_version":"1.0","canonical_sha256":"a7091e2da0b12a240f6d344b97a14d7cfe0450e25cadab235e8a6f0955a5a1a5","source":{"kind":"arxiv","id":"2101.03602","version":2},"attestation_state":"computed","paper":{"title":"Deploying heavier $\\eta$ meson states: configurational entropy hybridizing AdS/QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Roldao da Rocha","submitted_at":"2021-01-10T18:57:27Z","abstract_excerpt":"The meson family of $\\eta$ pseudoscalars is studied in the context of the AdS/QCD correspondence and the differential configurational entropy (DCE). For it, two forms of configurational-entropic Regge-like trajectories are engendered, relating the $\\eta$ mesonic states excitation number to both their experimental mass spectrum in the Particle Data Group (PDG) and the DCE as well. Hence, the mass spectrum of $\\eta$ pseudoscalar mesonic states, beyond the already detected states $\\eta(550)$, $\\eta'(958)$, $\\eta(1295)$, $\\eta(1405)$, $\\eta(1475)$, $\\eta(1760)$, $\\eta(2225)$, and $\\eta(2320)$, is "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2101.03602","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-01-10T18:57:27Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"45d6189c680f0b75149dc0e3044722d249cb9e7a055245f79a75be5b326b34bc","abstract_canon_sha256":"4423d9525d0dc80ea15c72d39a115198bb25b8ced9c487edde0f248a4a802875"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:12:31.805284Z","signature_b64":"oOq3Ifv1N0Lied27D15uVFOZPL1aBPjsmHQv7P6pDX18Pjp9Ly7xkLeYrscGPl5tJkMwyMqwk6KEyr6VTZxdBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a7091e2da0b12a240f6d344b97a14d7cfe0450e25cadab235e8a6f0955a5a1a5","last_reissued_at":"2026-07-05T02:12:31.804875Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:12:31.804875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deploying heavier $\\eta$ meson states: configurational entropy hybridizing AdS/QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Roldao da Rocha","submitted_at":"2021-01-10T18:57:27Z","abstract_excerpt":"The meson family of $\\eta$ pseudoscalars is studied in the context of the AdS/QCD correspondence and the differential configurational entropy (DCE). For it, two forms of configurational-entropic Regge-like trajectories are engendered, relating the $\\eta$ mesonic states excitation number to both their experimental mass spectrum in the Particle Data Group (PDG) and the DCE as well. Hence, the mass spectrum of $\\eta$ pseudoscalar mesonic states, beyond the already detected states $\\eta(550)$, $\\eta'(958)$, $\\eta(1295)$, $\\eta(1405)$, $\\eta(1475)$, $\\eta(1760)$, $\\eta(2225)$, and $\\eta(2320)$, is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.03602","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2101.03602/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2101.03602","created_at":"2026-07-05T02:12:31.804931+00:00"},{"alias_kind":"arxiv_version","alias_value":"2101.03602v2","created_at":"2026-07-05T02:12:31.804931+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.03602","created_at":"2026-07-05T02:12:31.804931+00:00"},{"alias_kind":"pith_short_12","alias_value":"U4ER4LNAWEVC","created_at":"2026-07-05T02:12:31.804931+00:00"},{"alias_kind":"pith_short_16","alias_value":"U4ER4LNAWEVCID3N","created_at":"2026-07-05T02:12:31.804931+00:00"},{"alias_kind":"pith_short_8","alias_value":"U4ER4LNA","created_at":"2026-07-05T02:12:31.804931+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.02375","citing_title":"Deformed AdS/QCD, mesonic mass spectra, and DCE: Still a margin for heavier resonances","ref_index":29,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT","json":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT.json","graph_json":"https://pith.science/api/pith-number/U4ER4LNAWEVCID3NGRFZPIKNPT/graph.json","events_json":"https://pith.science/api/pith-number/U4ER4LNAWEVCID3NGRFZPIKNPT/events.json","paper":"https://pith.science/paper/U4ER4LNA"},"agent_actions":{"view_html":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT","download_json":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT.json","view_paper":"https://pith.science/paper/U4ER4LNA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2101.03602&json=true","fetch_graph":"https://pith.science/api/pith-number/U4ER4LNAWEVCID3NGRFZPIKNPT/graph.json","fetch_events":"https://pith.science/api/pith-number/U4ER4LNAWEVCID3NGRFZPIKNPT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT/action/storage_attestation","attest_author":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT/action/author_attestation","sign_citation":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT/action/citation_signature","submit_replication":"https://pith.science/pith/U4ER4LNAWEVCID3NGRFZPIKNPT/action/replication_record"}},"created_at":"2026-07-05T02:12:31.804931+00:00","updated_at":"2026-07-05T02:12:31.804931+00:00"}